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November 1, 1967The Physics of Fluids224 citations

Turbulence Transport Equations

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FHFrancis H. HarlowPNP. I. Nakayama

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Abstract

A generalized eddy viscosity function σ, is introduced in order that the Reynolds stress in an incompressible fluid be expressible as a linear combination of the Kronecker and rate-of-strain tensors. A transport equation for the eddy viscosity is derived from the general turbulence energy equation, thereby introducing two additional functions, the specific turbulence kinetic energy q, and a scale variable s. To determine the three variables, a transport equation for s is postulated, and a modified Prandtl—Wieghardt relation among the three variables is accepted. The theory is expressed in universal, invariant form, and validity is demonstrated by application to several problems.

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Harlow et al. (1967) studied this question.

synapsesocial.com/papers/6a1de253cd67cee37334f97ehttps://doi.org/10.1063/1.1762039
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